Journal of Inequalities in Pure and Applied Mathematics http://jipam.vu.edu.au/ Volume 7, Issue 3, Article 116, 2006 SOME INEQUALITIES FOR SPECTRAL VARIATIONS SHILIN ZHAN D EPARTMENT OF M ATHEMATICS H ANSHAN T EACHER ’ S C OLLEGE C HAOZHOU , G UANGDONG , C HINA , 521041 shilinzhan@163.com Received 01 March, 2006; accepted 20 June, 2006 Communicated by B. Yang A BSTRACT. Over the last couple of decades, significant progress for the spectral variation of a matrix has been made in partially extending the classical Weyl and Lidskii theory [11, 7] to normal matrices and even to diagonalizable matrices for example. Recently these theories have been established for relative perturbations. In this paper, we shall establish relative perturbation theorems for generalized normal matrix. Some well-known perturbation theorems for normal matrix are extended. As applying, some perturbation theorems for positive definite matrix (possibly non-Hermitian) are established. Key words and phrases: Spectral variation; Unitarily invariant norm; Hadamard product; Relative perturbation theorem. 2000 Mathematics Subject Classification. 15A18, 15A42, 65F15. 1. I NTRODUCTION The set of all λ ∈ C that are eigenvalues of A ∈ Mn (C) is called the spectrum of A and is denoted by σ(A). The spectral radius of A is the nonnegative real number ρ(A) = max{|λ| : λ ∈ σ(A)}. We shall use k|·|k to denote a unitarily invariant norm (see [5, 9, 13, 3, 20, 21]). kXk2 , the largest singular value of X, is a frequently used unitarily invariant norm. Let X ◦Y = (xij yij ) be the Hadamard product of X = (xij ) and Y = (yij ). A matrix A ∈ Mn (C) is said to be a generalized normal matrix with respect to H (It is called “generalized normal matrix” for short) or H + -normal if there exists a positive definite Hermitian matrix H such that A∗ HA = AHA∗ , where “*” denotes the conjugate transpose. The definition was given first by [19, 18]. A generalized normal matrix is a very important kind of matrix which contains two subclasses of important matrices: normal matrices and positive definite matrices (possibly non-Hermitian), where a matrix A is called normal if A∗ A = AA∗ and positive definite if Re(x∗ Ax) > 0 for any non-zero x ∈ C n (see [5, 6]). In recent years, the geometric significance, sixty-two equivalent conditions and many properties have been established for generalized normal matrices in [19, 17, 18]. We have ISSN (electronic): 1443-5756 c 2006 Victoria University. All rights reserved. Research supported by the NSF of Guangdong Province (04300023) and NSF of Education Commission of Guangdong Province (Z03095). 060-06 2 S HILIN Z HAN Lemma 1.1 (see [19]). Suppose A ∈ Mn (C). Then (1) A is a generalized normal matrix with respect to H if and only if H 1/2 AH 1/2 is normal. (2) A is a generalized normal matrix with respect to H if and only if there exists a nonsingular matrix P such that H = (P P ∗ )−1 and A = P ΛP ∗ , (1.1) where Λ = diag(λ1 , λ2 , . . . , λn ). Furthermore, λ1 , λ2 , . . . , λn are n eigenvalues of HA. Remark 1.2. (1.1) is equivalent to HA = P −∗ ΛP ∗ with P −∗ = (P −1 )∗ , so we say that A has generalized eigen-decomposition (1.1), and λ1 , λ2 , . . . , λn are the generalized eigenvalues of matrix A. The spectral variation of a matrix has recently been a very active research subject in both matrix theory and numerical linear algebra. Over the last couple of decades significant progress has been made in partially extending the classical Weyl and Lidskii theory [11, 16] to normal matrices and even to diagonalizable matrices for example. This note will show how certain perturbation problems can be reformulated as simple matrix optimization problems involving Hadamard products. When A and à are normal, we have shown one of many perturbation theorems that can be interpreted as bounding the norms of Q◦Z where Q is unitary and Z is a special matrix defined by the eigenalues (see [10]). In this paper, we shall extend the above result, and shall show how certain perturbation problems can be reformulated as generalized normal matrix optimization problems involving Hadamard products. Also, we study how generalized eigenvalues of a generalized normal matrix A change when it is perturbed to à = D∗ AD, where D is a nonsingular matrix. As applications, some perturbation theorems for positive definite matrices (possibly non-Hermitian) are established. 2. M AIN R ESULT Suppose that A and à are generalized normal matrices with respect to a common positive definite matrix H, and have generalized eigen-decompositions A = P ΛP ∗ and Λ = diag(λ1 , λ2 , . . . , λn ) and (2.1) à = P̃ Λ̃P̃ ∗ , where (2.2) Λ̃ = diag(λ̃1 , λ̃2 , . . . , λ̃n ) and λi are the generalized eigenvalues of A, and λ̃i are the generalized eigenvalues of à (i = 1, 2, . . . , n). Notice H = (P P ∗ )−1 and H = (P̃ P̃ ∗ )−1 , so (P −1 P̃ )∗ (P −1 P̃ ) = P̃ ∗ H P̃ = I, then Q = P −1 P̃ is unitary and (2.3) P̃ = P Q Define (2.4) n Z1 = λi − λ̃j . i,j=1 We have the following result. Theorem 2.1. Suppose A and à are H + -normal with generalized eigen-decomposition (2.1), Then −1 (2.5) ρ(H) k|Q ◦ Z1 |k ≤ A − à ≤ ρ(H −1 ) k|Q ◦ Z1 |k , where Q = P −1 P̃ is unitary and Z1 is defined in Eq.(2.4). J. Inequal. Pure and Appl. Math., 7(3) Art. 116, 2006 http://jipam.vu.edu.au/ I NEQUALITIES FOR S PECTRAL VARIATIONS 3 Proof. For A and à having generalized eigen-decomposition (2.1), noticing that P̃ = P Q, where Q = P −1 P̃ is unitary, k|W Y |k ≤ kW k2 k|Y |k and k|Y Z|k ≤ k|Y |k kZk2 (see [9, p. 961]), we have ∗ ∗ ∗ ∗ P ΛP − P QΛ̃Q P ≤ kP k2 Λ − QΛ̃Q kP ∗ k2 , then Since A − à ≤ H −1 2 Λ − QΛ̃Q∗ . ∗ Λ − QΛ̃Q = ΛQ − QΛ̃ = k|Q ◦ Z1 |k and kH −1 k2 = ρ(H −1 ), A − à ≤ ρ(H −1 ) k|Q ◦ Z1 |k . (2.6) On the other hand, we have −1 ∗ ∗ ∗ −∗ ∗ P P ΛP − P Q Λ̃Q P Λ − Q Λ̃Q P ≥ 2 2 = k|Q ◦ Z1 |k . p Similarly for H = (P P ∗ )−1 and kP −1 k2 = kP −∗ k2 = ρ(H), we obtain ρ(H) A − à ≥ k|Q ◦ Z1 |k , hence A − à ≥ ρ(H)−1 k|Q ◦ Z1 |k . (2.7) The inequality (2.5) completes the proof by inequalities (2.6) and (2.7). In particular, if H = I is the identity matrix, then H + -normal matrices A and à are normal matrices, hence A and à have eigen-decomposition A = U ΛU ∗ (2.8) and à = Ũ Λ̃Ũ ∗ , where U and Ũ are unitary, and Λ = diag(λ1 , λ2 , . . . , λn ), Λ̃ = diag(λ̃1 , λ̃2 , . . . , λ̃n ). By Theorem 2.1, we have Corollary 2.2 (see [10]). If A and à are normal matrices, then (2.9) A − à = k|Q ◦ Z1 |k , n . where Q = U ∗ Ũ and Z1 = λi − λ̃j i,j=1 We denote the Cartesian decomposition X = H(X) + K(X), where H(X) = 12 (X + X ∗ ), and K(X) = 12 (X − X ∗ ). Let σ (H (A)) = {h1 , h2 , . . . , hn } be ordered so that h1 ≥ h2 ≥ · · · ≥ hn . Then we have some perturbation theorems for positie definite matrices which are discussed as follows. Corollary 2.3. If A = H(A) + K(A) and à = H(Ã) + K(Ã) are positive definite with generalized eigen-decomposition (2.1), and Q = P −1 P̃ is unitary, then (2.10) hn k|Q ◦ Z1 |k ≤ A − à ≤ h1 k|Q ◦ Z1 |k , where Z1 is defined in Eq.(2.4). J. Inequal. Pure and Appl. Math., 7(3) Art. 116, 2006 http://jipam.vu.edu.au/ 4 S HILIN Z HAN Proof. Since Q = P −1 P̃ is unitary, H(A) = H(Ã). It is easy to see that A∗ H(A)−1 A = AH(A)−1 A∗ and Ã∗ H(Ã)−1 à = ÃH(Ã)−1 Ã∗ . So A and à are generalized normal matrices with respect to H(A)−1 . It is easy to see that ρ(H(A)−1 )−1 = hn , ρ(H(A)) = h1 . Applying Theorem 2.1, inequality (2.10) completes the proof. Let B, C ∈ Mn (C). Then [B, C] = BC − CB is called a commutator and [B, C]H = BHC − CHB is called a commutator with respect to H. The matrices B and C are said to commute with respect to H iff [B, C]H = 0. kXkF is the Frobenius norm. Corollary 2.4. Let A and à be H + -normal matrices. If A and à commute with respect to H, then −1 (2.11) ρ(H) k|I ◦ Z1 |k ≤ A − à ≤ ρ(H −1 ) k|I ◦ Z1 |k , where I is the identity matrix, and Z1 is defined in Eq.(2.4). Proof. [A, Ã]H = 0 if and only if there exists a nonsingular matrix P , such that A = P ΛP ∗ and à = P Λ̃P ∗ , where Q = P −1 P = I (see [17, Theorem 3] and Theorem 2.1). So Q is taken as the identity matrix I in Theorem 2.1, hence Eq. (2.11) holds. Applying Corollary 2.3 and Corollary 2.4, we have Corollary 2.5. Let the hypotheses of Corollary 2.3 hold. Moreover if matrices A and à commute with respect to H(A)−1 , then (2.12) hn k|I ◦ Z1 |k ≤ A − à ≤ h1 k|I ◦ Z1 |k , where h1 = max1≤i≤n λi (H(A)), hn = min1≤i≤n λi (H(A)) and Z1 is defined in Eq.(2.4). In the following, we shall study how generalized eigenvalues of a generalized normal matrix A change when it is perturbed to à = D∗ AD, where D is a nonsingular matrix. The p−relative distance between α, α̃ ∈ C is defined as |α − α̃| %p (α, α̃) = p p (2.13) |α|p + |α̃|p for 1 ≤ p ≤ ∞. Theorem 2.6. Suppose A and à are H + -normal matrices and à = D∗ AD, where D is nonsingular. Let A and à have generalized eigen-decomposition (2.1). Then there is a permutation τ of {1, 2, . . . , n} such that n X (2.14) 2 [%2 (λi , λ̃τ (i) )]2 ≤ c(kI − Dk2F + D−∗ − I F ) i=1 where c = max1≤i≤n λi (H)/ min1≤i≤n λi (H). Proof. Notice that A − à = A − D∗ AD = A(I − D) + (D−∗ − I)Ã. Pre- and postmultiply the equations by P −1 and P̃ −∗ respectively, to get (2.15) ΛP ∗ P̃ −∗ − P −1 P̃ Λ̃ = ΛP ∗ (I − D)P̃ −∗ + P −1 (D−∗ − I)P̃ Λ̃. J. Inequal. Pure and Appl. Math., 7(3) Art. 116, 2006 http://jipam.vu.edu.au/ I NEQUALITIES FOR S PECTRAL VARIATIONS 5 Set Q = P −1 P̃ = (qij ), then Q is unitary and Q = P ∗ P̃ −∗ . Let (2.16) E = P ∗ (I − D)P̃ −∗ = (eij ), Ẽ = P −1 (D−∗ − I)P̃ = (ẽij ). Then (2.15) implies that ΛQ− QΛ̃ = ΛE + Ẽ Λ̃ or componentwise λi qij − qij λ̃j = λi eij + ẽij λ̃j , so 2 2 2 2 2 2 (λi − λ̃j )qij = λi eij + ẽij λ̃j ≤ (|λi | + λ̃j )(|eij | + |ẽij | ), which yields [%2 (λi , λ̃j )]2 |qij |2 ≤ |eij |2 + |ẽij |2 . Hence n X [%2 (λi , λ̃j )]2 |qij |2 i,j=1 2 2 ∗ −1 −∗ −∗ ≤ P (I − D)P̃ + P (D − I)P̃ F F 2 2 2 2 2 2 ∗ −∗ −1 −∗ ≤ kP k2 kI − DkF P̃ + P D − I F P̃ . 2 2 2 Notice that kP ∗ k22 = max λi (H) and 1≤i≤n −1 2 P = 2 −1 min λi (H) 1≤i≤n 2 by σ(P P ∗ ) = σ(P ∗ P ) = σ(H). Similarly, we have P̃ = max1≤i≤n λi (H) and 2 −∗ 2 P̃ = max1≤i≤n λi (H −1 ) = 2 −1 min λi (H) , 1≤i≤n so n h X i2 2 %2 λi , λ̃j |qij |2 ≤ c kI − Dk2F + D−∗ − I F , i,j=1 where c = max1≤i≤nλi (H)/min1≤i≤n λi (H). The matrix |qij |2 n×n is a doubly stochastic matrix. The above inequality and [9, Lemma 5.1] imply inequality (2.14). If A and à are normal matrices, then they are generalized normal matrices with respect to H and H = I. Applying Theorem 2.6, it is easy to get Corollary 2.7. If A, à ∈ Mn (C) are normal matrices with A = U ΛU ∗ and à = Ũ Λ̃Ũ ∗ where both U and Ũ are unitary, and à = D∗ AD, where D is nonsingular, then n X (2.17) 2 [%2 (λi , λ̃τ (i) )]2 ≤ kI − Dk2F + D−∗ − I F . i=1 Corollary 2.8. Let A = H(A) + K(A) and à = H(Ã) + K(Ã) be positive definite matrices with generalized eigen-decomposition (2.1), and à = D∗ AD, where D is nonsingular. If Q = P −1 P̃ is unitary, then n h i2 X 2 (2.18) %2 λi , λ̃τ (i) ≤ c kI − Dk2F + D−∗ − I F , i,=1 where c = max 1≤i≤n λi (H(A))/ min 1≤i≤n λi (H(A)). J. Inequal. Pure and Appl. Math., 7(3) Art. 116, 2006 http://jipam.vu.edu.au/ 6 S HILIN Z HAN Proof. By the proof of Corollary 2.3, A and à are generalized normal matrices with respect to H(A)−1 , and max λi (H(A)−1 )/ min λi (H(A)−1 ) = max λi (H(A))/min1≤i≤n λi (H(A)). 1≤i≤n 1≤i≤n 1≤i≤n Inequality (2.18) is proved by Theorem 2.6. R EFERENCES [1] T. ANDO, R.A. HORN AND C.R. JOHNSON, The singular values of a Hadamard product: a basic inequality, Linear and Multilinear Algebra, 87 (1987), 345–365. [2] S.C. EISENSTAT AND I.C.F. IPSEN, Three absolute perturbation bounds for matrix eigenvalues imply relative bounds, SIAM J. Matrix Anal. Appl., 20 (1999). [3] F. HIAI AND X. ZHAN, Inequalities involving unitarily invariant norms and operator monotone functions, Linear Algebra Appl., 341 (2002), 151–169. [4] J.A. 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